Abstract

This paper presents an experimental study of the influence of heat losses on the onset of thermoacoustic instabilities in methane–air premixed flames propagating in a horizontal tube of diameter,$D = 10$mm. Flames are ignited at the open end of the tube and propagate towards the closed end undergoing strong oscillations of different features owing to the interaction with acoustic waves. The frequency of oscillation and its axial location are controlled through the tube length$L$and the intensity of heat losses. These parameters are respectively modified in the experiments by a moveable piston and a circulating thermal bath of water prescribing temperature conditions. Main experimental observations show that classical one-dimensional predictions of the oscillation frequency do not accurately describe the phenomena under non-adiabatic real scenarios. In addition to the experimental measurements, a quasi-one-dimensional analysis of the burnt gases is provided, which introduces the effect of heat losses at the wall of the tube on the interplay between the acoustic field and the reaction sheet. As a result, this analysis provides an improved description of the interaction and accurately predicts the excited flame-oscillation harmonics through the eigenvalues of the non-adiabatic acoustics model. Unlike the original one-dimensional analysis, the comparison between the flame oscillation frequency provided by the non-adiabatic extended theory and the frequencies measured in our experiments is in excellent agreement in the whole range of temperatures considered. This confirms the importance of heat losses in the modulation of the instabilities and the transition between different flame oscillation regimes.

Highlights

  • Premixed flame propagation is a rich problem that has been fruitfully addressed for many years by the scientific community

  • Thermoacoustic coupling in tubes has been a field of intense study since the original reports by Sondhauss (1850), which dealt with external heating of pipes with a closed end, and by Rijke (1859) that covered heated tubes with two open ends

  • The present study focuses on intermediate scenarios, moderate tube diameters that prevent the growth of large-scale dynamic instabilities of the flow, and which characteristically sit far from negligible heat losses in the averaged section

Read more

Summary

Introduction

Premixed flame propagation is a rich problem that has been fruitfully addressed for many years by the scientific community. Regardless of the heat release source, this interaction was first explained by Rayleigh (1878) through his thermoacoustic growth criterion: heat promotes acoustic waves if released at the compression stage or if extracted during rarefaction. This behaviour was detected early on burners by Mallard & Le Chatelier (1881) and later addressed experimentally (Mason & Wheeler 1920; Coward, Hartwell & Georgeson 1937), where the marked behaviour of oscillating flames under smooth and violent regimes was directly related to acoustic coupling. In region 0 < ξ < r, the properties of the gas are those of the quiescent unburnt mixture, that is, density ρu and temperature Tu, and the region

Results
Discussion
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call